This patterning was reproduced by Duguet et al. [1]}
using fully resolved numerical simulations in an extended system of size comparable with that of the Saclay apparatus but the computational load
was so heavy that a statistical study of the upper transitional range was inconceivable. Earlier, Barkley & Tuckerman [2]} also succeeded
in obtaining the bands by means of fully resolved simulations with less
computational burden but using narrow elongated domains aligned with
the pattern's wavevector.
By construction, the fluctuating domain regime could not be obtained,
whereas a re-entrant
featureless turbulence regime, called `intermittent' was obtained closer
to \(R_{\rm t}\) .
